2017
DOI: 10.1049/el.2016.4163
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Micro‐Doppler detection in forward scattering radar: theoretical analysis and experiment

Abstract: Forward scatter radar (FSR) is actively studied in the field of radars, as it has many advantages such as robust to radar absorbing material and possibility in target recognition. In many radar systems, micro-Doppler signature is one of the most distinguished information used for target recognition. Yet, there is lacking in established work on investigating the feasibility of using FSR to detect and analyse micro-Doppler signature generated from micro-motions of moving targets. Hence, a theoretical and experim… Show more

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Cited by 6 publications
(5 citation statements)
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“…Typically, N is 2 for drone/UAV/quadcopter propeller and it varies from 2 to 6 for helicopters of different radar cross-section (RCS) and payload capacity [13,14,25]. More than one rotating target or a target having multiple rotating parts can be distinguished based on the micro-Doppler frequency and range profiles generated by them [13,26,27]. Whole body and parts of a walking/jogging/cycling person can be distinguished by carefully analysing the micro-Doppler spectral signatures [21,28].…”
Section: Background Conceptsmentioning
confidence: 99%
“…Typically, N is 2 for drone/UAV/quadcopter propeller and it varies from 2 to 6 for helicopters of different radar cross-section (RCS) and payload capacity [13,14,25]. More than one rotating target or a target having multiple rotating parts can be distinguished based on the micro-Doppler frequency and range profiles generated by them [13,26,27]. Whole body and parts of a walking/jogging/cycling person can be distinguished by carefully analysing the micro-Doppler spectral signatures [21,28].…”
Section: Background Conceptsmentioning
confidence: 99%
“…When the pendulum exactly crosses the baseline, the frequency and amplitude of Doppler signature are equal to zero. At the baseline the Doppler frequency equals zero because the bistatic angle β pen equals 180 • as depicted in Equation 4, and the amplitude becomes minimum or zero because the direct and scattered signals are equal and opposite each other in phase [18]. The BL crossing points are marked by circles.…”
Section: Doppler Frequency Generated From One Pendulum Swinging On Fsmentioning
confidence: 99%
“…where is the tangential velocity of the pendulum, which is previously given in (18), and is the translational motion due to the linear motion of the pendulum's assembly point (pivot In this case, the pivot of pendulum p moves linearly from y max to −y max along the Y-axis while the pendulum mass is swinging. Therefore, the coordinates of pendulum mass changes with time due to: (i) the vibration motion of pendulum; and (ii) the straight motion because of linear translation motion of its pivot point p. In Figure 4, the instantaneous translational coordinates of the pendulum mass are as follows:…”
Section: Micro-doppler Frequency Generated From One Swinging Pendulummentioning
confidence: 99%
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